1,532 research outputs found

    Thermodynamical behaviour of the Variable Chaplygin gas

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    The thermodynamical behaviour of the Variable Chaplygin gas (VCG) model is studied, using an equation of state like P=BρP = - \frac{B}{\rho}, where B=B0Vn3B = B_{0}V^{-\frac{n}{3}}. Here B0B_{0} is a positive universal constant, nn is also a constant and VV is the volume of the fluid. From the consideration of thermodynamic stability, it is seen that only if the values of nn are allowed to be negative, then (PV)S<0(\frac{\partial P}{\partial V})_{S} <0 throughout the evolution. Again thermal capacity at constant volume cVc_{V} shows positive expression. Using the best fit value of n=3.4 n = -3.4 as previously found by Guo \emph{et al} \cite{guo1} gives that the fluid is thermodynamically stable through out the evolution. The effective equation of state for the special case of, n=0n = 0 goes to Λ\LambdaCDM model. Again for n<0n <0 it favours phantom-like cosmology which is in agreement with the current SNe Ia constraints like VCG model. The deceleration parameter is also studied in the context of thermodynamics and the analysis shows that the \emph{flip} occurs for the value of n<4 n < 4. Finally the thermal equation of state is discussed which is an explicit function of temperature only. It is also observed that the third law of thermodynamics is satisfied in this model. As expected the volume increases as temperature falls during adiabatic expansions. In this case, for T0 T \rightarrow 0, the thermal equation of state reduces to (1+n6)(- 1 + \frac{n}{6}) which is identical with the equation of state for the case of large volume.Comment: 10 pages, 4 figure

    Thermodynamics of the Variable Modified Chaplygin gas

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    A cosmological model with a new variant of Chaplygin gas obeying an equation of state(EoS), P=AρBραP = A\rho - \frac{B}{\rho^{\alpha}} where B=B0anB= B_{0}a^{n} is investigated in the context of its thermodynamical behaviour. Here B0B_{0} and nn are constants and aa is the scale factor. We show that the equation of state of this `Variable Modified Chaplygin gas' (VMCG) can describe the current accelerated expansion of the universe. Following standard thermodynamical criteria we mainly discuss the classical thermodynamical stability of the model and find that the new parameter, nn introduced in VMCG plays a crucial role in determining the stability considerations and should always be \emph{negative.} We further observe that although the earlier model of Lu explains many of the current observational findings of different probes it fails the desirable tests of thermodynamical stability. We also note that for n<0n < 0 our model points to a phantom type of expansion which, however, is found to be compatible with current SNe Ia observations and CMB anisotropy measurements. Further the third law of thermodynamics is obeyed in our case. Our model is very general in the sense that many of earlier works in this field may be obtained as a special case of our solution. An interesting point to note is that the model also apparently suggests a smooth transition from the big bang to the big rip in its whole evaluation process.Comment: 19 pages, 8 figure

    Energy dissipation in wave propagation in general relativistic plasma

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    Based on a recent communication by the present authors the question of energy dissipation in magneto hydrodynamical waves in an inflating background in general relativity is examined. It is found that the expanding background introduces a sort of dragging force on the propagating wave such that unlike the Newtonnian case energy gets dissipated as it progresses. This loss in energy having no special relativistic analogue is, however, not mechanical in nature as in elastic wave. It is also found that the energy loss is model dependent and also depends on the number of dimensions.Comment: 12 page

    Quintessential Phenomena in Higher Dimensional Space Time

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    The higher dimensional cosmology provides a natural setting to treat, at a classical level, the cosmological effects of vacuum energy. Here we discuss two situations where starting with an ordinary matter field without any equation of state we end up with a Chaplygin type of gas apparently as a consequence of extra dimensions. In the second case we study the quintessential phenomena in higher dimensional spacetime with the help of a Chaplygin type of matter field. The first case suffers from the disqualification that no dimensional reduction occurs, which is, however, rectified in the second case. Both the models show the sought after feature of occurrence of \emph{flip} in the rate of expansion. It is observed that with the increase of dimensions the occurrence of \emph{flip} is delayed for both the models, more in line with current observational demands. Interestingly we see that depending on some initial conditions our model admits QCDM, Λ\LambdaCDM and also Phantom like evolution within a unified framework. Our solutions are general in nature in the sense that when the extra dimensions are switched off the known 4D model is recovered.Comment: 17 Pages, 7 figure

    Controlled transportation of mesoscopic particles by enhanced spin orbit interaction of light in an optical trap

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    We study the effects of the spin orbit interaction (SOI) of light in an optical trap and show that the propagation of the tightly focused trapping beam in a stratified medium can lead to significantly enhanced SOI. For a plane polarized incident beam the SOI manifests itself by giving rise to a strong anisotropic linear diattenuation effect which produces polarization-dependent off-axis high intensity side lobes near the focal plane of the trap. Single micron-sized asymmetric particles can be trapped in the side lobes, and transported over circular paths by a rotation of the plane of input polarization. We demonstrate such controlled motion on single pea-pod shaped single soft oxometalate (SOM) particles of dimension around 1×0.5μ1\times 0.5\mum over lengths up to \sim15 μ\mum . The observed effects are supported by calculations of the intensity profiles based on a variation of the Debye-Wolf approach. The enhanced SOI could thus be used as a generic means of transporting mesoscopic asymmetric particles in an optical trap without the use of complex optical beams or changing the alignment of the beam into the trap.Comment: 9 pages, 7 figure

    Diffraction limit of the sub-Planck structures

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    The orthogonality of cat and displaced cat states, underlying Heisenberg limited measurement in quantum metrology, is studied in the limit of large number of states. The asymptotic expression for the corresponding state overlap function, controlled by the sub-Planck structures arising from phase space interference, is obtained exactly. The validity of large phase space support, in which context the asymptotic limit is achieved, is discussed in detail. For large number of coherent states, uniformly located on a circle, it identically matches with the diffraction pattern for a circular ring with uniform angular source strength. This is in accordance with the van Cittert-Zernike theorem, where the overlap function, similar to the mutual coherence function matches with a diffraction pattern.Comment: 5 pages, 3 figure

    Proper acceleration, geometric tachyon and dynamics of a fundamental string near Dpp branes

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    We present a detailed analysis of our recent observation that the origin of the geometric tachyon, which arises when a Dpp-brane propagates in the vicinity of a stack of coincident NS5-branes, is due to the proper acceleration generated by the background dilaton field. We show that when a fundamental string (F-string), described by the Nambu-Goto action, is moving in the background of a stack of coincident Dpp-branes, the geometric tachyon mode can also appear since the overall conformal mode of the induced metric for the string can act as a source for proper acceleration. We also studied the detailed dynamics of the F-string as well as the instability by mapping the Nambu-Goto action of the F-string to the tachyon effective action of the non-BPS D-string. We qualitatively argue that the condensation of the geometric tachyon is responsible for the (F,Dpp) bound state formation.Comment: 26 pages, v2: added references, v3: one ref. updated, to appear in Class. and Quant. Gravit
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